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THESE de DOCTORAT - cerfacs

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7.2 Mean parameters of the Intake Duct 121<br />

system. At first, simplified acoustic boundary conditions are imposed at both inlet and outlet<br />

(u’=0). They can be consi<strong>de</strong>red as fully reflecting conditions as if they were a rigid wall. In<br />

a second step, the impedance computed by the SNozzle tool for the inlet of the combustion<br />

chamber is used instead of the simple u ′ = 0 condition.<br />

When the simple condition (u’=0) is used, the Helmholtz solver computes an acoustic mo<strong>de</strong><br />

around 500Hz which is consi<strong>de</strong>red a value far from what is observed in experiments. It is well<br />

known that the resonant mo<strong>de</strong>s of a system are fully <strong>de</strong>pen<strong>de</strong>nt on the acoustic boundary conditions<br />

used [56]. A viewpoint often put forward is that the bad prediction of the resonant<br />

frequency by the Helmholtz solver is probably due to the simplified treatment of acoustics<br />

at both the inlet and the outlet. In the combustion chamber studied, the flow is shocked at<br />

the outlet. In this case, and for low frequencies, it is known that the reflection coefficient can<br />

be consi<strong>de</strong>red close to that of a rigid wall. On the other hand, the same cannot be stated for<br />

the inlet. Acoustic properties of the combustion chamber inlet are fully <strong>de</strong>pen<strong>de</strong>nt on the upstream<br />

configuration of the combustor. The question that is investigated in this chapter is then<br />

whether a more accurate <strong>de</strong>scription of the inlet impedance leads to large changes in the mo<strong>de</strong><br />

computed by the Helmholtz solver, hopefully in better agreement with the experiments. This<br />

exercise also serves as an illustration of the capability of the SNozzle tool to represent complex<br />

intakes.<br />

Aeronautical engines are complex systems in which the combustion chamber is present just in a<br />

tiny region after the compressor stages. From the point of view of the combustor, the upstream<br />

region is then composed by several compression stages in which acoustics <strong>de</strong>pends on enthalpy<br />

jumps (compressors), the intake acoustic condition (usually related to the atmosphere) and<br />

the geometry of the entire system. Figure 7.1 shows the intake duct of a typical helicopter<br />

combustor.<br />

SNozzle has been <strong>de</strong>veloped for computing the acoustic response of a quasi-1D system to an<br />

acoustic perturbation. This numerical tool consi<strong>de</strong>rs non-negligible Mach numbers as well as<br />

total pressure jumps in the mean flow. SNozzle is then consi<strong>de</strong>red appropriate to evaluate the<br />

acoustic impedance at a specific transversal plane of systems, such as of the present aeronautical<br />

air-intake duct. Once the acoustic impedance is evaluated, this acoustic condition can be<br />

imposed in the Helmholtz solver. Resonant frequencies closer to the experimental measurements<br />

are expected. Insignificant changes in the computed mo<strong>de</strong> would support the i<strong>de</strong>a that<br />

the disagreement between the computed and observed mo<strong>de</strong> is not due to errors in the inlet<br />

impedance <strong>de</strong>scription.<br />

7.2 Mean parameters of the Intake Duct<br />

SNozzle needs two thermodynamical parameters (temperature and pressure) , the Mach number<br />

at the outlet (see Fig. 7.1) and the section area as a function of the curvilinear axis (Fig. 7.2).<br />

The position and the total pressure jump due to the compressors is also nee<strong>de</strong>d in or<strong>de</strong>r to

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